{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:SSWFHGVM2TDVARUVUXTIM2UHNF","short_pith_number":"pith:SSWFHGVM","canonical_record":{"source":{"id":"hep-ph/9811224","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-11-02T22:08:38Z","cross_cats_sorted":[],"title_canon_sha256":"87b82fa80ef01d54f674a89fa5fcbbc692f260ca79b0eb90f97053df3132d814","abstract_canon_sha256":"ca611ad538d0bf5909a5ff882a99edbba1b2cd1c65e470bad0bdf4a7ef0fe2b1"},"schema_version":"1.0"},"canonical_sha256":"94ac539aacd4c7504695a5e6866a8769740463e523025b34119e50ad90978c68","source":{"kind":"arxiv","id":"hep-ph/9811224","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9811224","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9811224v1","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9811224","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_12","alias_value":"SSWFHGVM2TDV","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_16","alias_value":"SSWFHGVM2TDVARUV","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_8","alias_value":"SSWFHGVM","created_at":"2026-07-04T16:09:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:SSWFHGVM2TDVARUVUXTIM2UHNF","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9811224","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-11-02T22:08:38Z","cross_cats_sorted":[],"title_canon_sha256":"87b82fa80ef01d54f674a89fa5fcbbc692f260ca79b0eb90f97053df3132d814","abstract_canon_sha256":"ca611ad538d0bf5909a5ff882a99edbba1b2cd1c65e470bad0bdf4a7ef0fe2b1"},"schema_version":"1.0"},"canonical_sha256":"94ac539aacd4c7504695a5e6866a8769740463e523025b34119e50ad90978c68","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:09:34.983140Z","signature_b64":"iiANPilOd34nahfJ6pz0AoZtT9MIiAhA8HEMWaieCwVKi0QN7GAsHOdZ/wFuU6Mfj18IliE4XCIDgl7Et0EEAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94ac539aacd4c7504695a5e6866a8769740463e523025b34119e50ad90978c68","last_reissued_at":"2026-07-04T16:09:34.982798Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:09:34.982798Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9811224","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ouf3tVoPcECai08x4C1YUexvCF59lsLdZwj0Wz7lh6L9ZI2cdV6CdsOaSZncopTCEIfFKS0gDGG2kdr2XNNHDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T21:32:34.106829Z"},"content_sha256":"3690ce3042f18347bf35550e191f1e3c1763091fbf9e9576cb1b73986ed218e2","schema_version":"1.0","event_id":"sha256:3690ce3042f18347bf35550e191f1e3c1763091fbf9e9576cb1b73986ed218e2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:SSWFHGVM2TDVARUVUXTIM2UHNF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalized Effective QCD Hamiltonian: Gluonic Sector","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C.-R. Ji, D. G. Robertson, E. S. Swanson (NCSU) A. P. Szczepaniak(IUB), S. R. Cotanch(NCSU)","submitted_at":"1998-11-02T22:08:38Z","abstract_excerpt":"Extending previous QCD Hamiltonian studies, we present a new renormalization procedure which generates an effective Hamiltonian for the gluon sector. The formulation is in the Coulomb gauge where the QCD Hamiltonian is renormalizable and the Gribov problem can be resolved. We utilize elements of the Glazek and Wilson regularization method but now introduce a continuous cut-off procedure which eliminates non-local counterterms. The effective Hamiltonian is then derived to second order in the strong coupling constant. The resulting renormalized Hamiltonian provides a realistic starting point for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9811224","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9811224/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:09:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kjI34/wROOvvZKwL24CEPH1hf/dL1jBxuNm9zpaiZiuGjaWqaysux5VibRJbUxSUqUJxaAILuW7n5q1gXgqJAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T21:32:34.107341Z"},"content_sha256":"c7a1f2bb47464e77ba5349cab8b066ab6f24f24558a207dba2431544f05591b9","schema_version":"1.0","event_id":"sha256:c7a1f2bb47464e77ba5349cab8b066ab6f24f24558a207dba2431544f05591b9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/bundle.json","state_url":"https://pith.science/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-10T21:32:34Z","links":{"resolver":"https://pith.science/pith/SSWFHGVM2TDVARUVUXTIM2UHNF","bundle":"https://pith.science/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/bundle.json","state":"https://pith.science/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SSWFHGVM2TDVARUVUXTIM2UHNF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:SSWFHGVM2TDVARUVUXTIM2UHNF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ca611ad538d0bf5909a5ff882a99edbba1b2cd1c65e470bad0bdf4a7ef0fe2b1","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-11-02T22:08:38Z","title_canon_sha256":"87b82fa80ef01d54f674a89fa5fcbbc692f260ca79b0eb90f97053df3132d814"},"schema_version":"1.0","source":{"id":"hep-ph/9811224","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9811224","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9811224v1","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9811224","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_12","alias_value":"SSWFHGVM2TDV","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_16","alias_value":"SSWFHGVM2TDVARUV","created_at":"2026-07-04T16:09:34Z"},{"alias_kind":"pith_short_8","alias_value":"SSWFHGVM","created_at":"2026-07-04T16:09:34Z"}],"graph_snapshots":[{"event_id":"sha256:c7a1f2bb47464e77ba5349cab8b066ab6f24f24558a207dba2431544f05591b9","target":"graph","created_at":"2026-07-04T16:09:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/9811224/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Extending previous QCD Hamiltonian studies, we present a new renormalization procedure which generates an effective Hamiltonian for the gluon sector. The formulation is in the Coulomb gauge where the QCD Hamiltonian is renormalizable and the Gribov problem can be resolved. We utilize elements of the Glazek and Wilson regularization method but now introduce a continuous cut-off procedure which eliminates non-local counterterms. The effective Hamiltonian is then derived to second order in the strong coupling constant. The resulting renormalized Hamiltonian provides a realistic starting point for","authors_text":"C.-R. Ji, D. G. Robertson, E. S. Swanson (NCSU) A. P. Szczepaniak(IUB), S. R. Cotanch(NCSU)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-11-02T22:08:38Z","title":"Renormalized Effective QCD Hamiltonian: Gluonic Sector"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9811224","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:3690ce3042f18347bf35550e191f1e3c1763091fbf9e9576cb1b73986ed218e2","target":"record","created_at":"2026-07-04T16:09:34Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ca611ad538d0bf5909a5ff882a99edbba1b2cd1c65e470bad0bdf4a7ef0fe2b1","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-11-02T22:08:38Z","title_canon_sha256":"87b82fa80ef01d54f674a89fa5fcbbc692f260ca79b0eb90f97053df3132d814"},"schema_version":"1.0","source":{"id":"hep-ph/9811224","kind":"arxiv","version":1}},"canonical_sha256":"94ac539aacd4c7504695a5e6866a8769740463e523025b34119e50ad90978c68","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"94ac539aacd4c7504695a5e6866a8769740463e523025b34119e50ad90978c68","first_computed_at":"2026-07-04T16:09:34.982798Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:09:34.982798Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iiANPilOd34nahfJ6pz0AoZtT9MIiAhA8HEMWaieCwVKi0QN7GAsHOdZ/wFuU6Mfj18IliE4XCIDgl7Et0EEAw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:09:34.983140Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9811224","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3690ce3042f18347bf35550e191f1e3c1763091fbf9e9576cb1b73986ed218e2","sha256:c7a1f2bb47464e77ba5349cab8b066ab6f24f24558a207dba2431544f05591b9"],"state_sha256":"931e2ff3e25e63a054c587a10de44c8ab9c0dae3fabb6d7e3c0f4fc3a33f5ec4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7qAA/crx8zj+qJm1u8xL/J7GFq7r1RBlewdEJ7C59tkj/wuVXc2DdGMchuJ5eMof/7Vestu3O4xsNnBr0LFsCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T21:32:34.111790Z","bundle_sha256":"b5d541a98bd014624dfd0e29b8e39909a622f1e361b3376213c4794091b15860"}}